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Table 3.

Spectral energy distribution fit results.

Epochs Modelc χ2/d.o.f. βlow βhigh Ebreak N(H, int)e E(B − V)e
(day) (keV) (1021 cm−2) (mag)
0.03a BPL 1.10 0 . 631 0.005 + 0.005 Mathematical equation: $ 0.631_{-0.005}^{+0.005} $ βlow + 0.5 2 . 09 0.05 + 0.08 Mathematical equation: $ 2.09_{-0.05}^{+0.08} $ 1.14 0.012
0.10a BPL 1.10 0 . 592 0.006 + 0.008 Mathematical equation: $ 0.592_{-0.006}^{+0.008} $ βlow + 0.5 2 . 63 0.33 + 0.42 Mathematical equation: $ 2.63_{-0.33}^{+0.42} $ 1.14 0.012
0.03b PL 2.3 0 . 59 0.004 + 0.006 Mathematical equation: $ 0.59_{-0.004}^{+0.006} $ 1.14 0.012
0.10b PL 1.4 0 . 62 0.006 + 0.006 Mathematical equation: $ 0.62_{-0.006}^{+0.006} $ 1.14 0.012

0.24–1.50d PL 0.99 0 . 705 0.005 + 0.004 Mathematical equation: $ 0.705_{-0.005}^{+0.004} $ 1 . 14 0.28 + 0.26 Mathematical equation: $ 1.14_{-0.28}^{+0.26} $ 0.012 ± 0.009

Notes.

a

These two SEDs share extinction and dust absorption from later epochs, but the spectral-model parameters are left free.

b

Similar to a but using a single power law model.

c

We use two models: a broken power law (BPL) and a power law (PL).

d

Joint fit: These two SEDs share the same model, and only the normalisation is left free.

e

The first four SEDs have the same N(H, int) and E(B − V), fixed to the values found in the late-time fit.

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